2010/05/11 by S. Ovchinnikov, Ovchinnikov, S., Yu. Orlov +5
Physics and Astronomy · #FOS: Physical sciences #Strongly Correlated Electrons (cond-mat.str-el) #cond-mat.str-el
paper · pdf · doi:10.48550/arxiv.1005.1732
arxiv created 2010/05/11 · arxiv updated 2010/05/12
For many years a spin-state transition at T ≈ 100 K and insulator - metal transition (IMT) at TIMT ≈ 600 K in LaCoO3 remains a mystery. Small low-spin - high-spin spin gap ΔS = E( HS ) - E( LS ) ∼ 100 K results in the spin-state transition. The large charge gap 2Ea ≈ 2300 K (Ea is the activation energy) vs. ΔS and TIMT implies that LaCoO3 is not a simple narrow-gap semiconductor. Here we explain both the spin-state and IMT on the same footing. We obtain strong temperature dependent band structure in LaCoO3 by the LDA+GTB method that incorporates strong electron correlations, covalence and spin-orbital interaction exactly inside the CoO6 cluster and the interclaster hopping between different multielectron configurations by perturbation theory for Hubbard X-operators.